Two level systems that can be reliably controlled and measured hold promise as qubits both for metrology and for quantum information science (QIS). Since a fluctuating environment limits the performance of qubits in both capacities, understanding the environmental coupling and dynamics is key to improving qubit performance. We show measurements of the level splitting and dephasing due to voltage noise of a GaAs singlet-triplet qubit during exchange oscillations. Unexpectedly, the voltage fluctuations are non-Markovian even at high frequencies and exhibit a strong temperature dependence. The magnitude of the fluctuations allows the qubit to be used as a charge sensor with a sensitivity of 2 × 10 −8 e/ √ Hz, two orders of magnitude better than a quantum-limited RF single electron transistor (RF-SET). Based on these measurements we provide recommendations for improving qubit coherence, allowing for higher fidelity operations and improved charge sensitivity. Two level quantum systems (qubits) are emerging as promising candidates both for quantum information processing [1] and for sensitive metrology [2,3]. When prepared in a superposition of two states and allowed to evolve, the state of the system precesses with a frequency proportional to the splitting between the states. However, on a timescale of the coherence time, T 2 , the qubit loses its quantum information due to interactions with its noisy environment. This causes qubit oscillations to decay and limits the fidelity of quantum control and the precision of qubit-based measurements. In this work we study singlet-triplet (S-T 0 ) qubits, a particular realization of spin qubits [4][5][6][7][8][9][10][11], which store quantum information in the joint spin state of two electrons [12][13][14]. We form the qubit in two gate-defined lateral quantum dots (QD) in a GaAs/AlGaAs heterostructure (Fig. 1a). The QDs are depleted until there is exactly one electron left in each, so that the system occupies the so-called (1, 1) charge configuration. Here (n L , n R ) describes a double QD with n L electrons in the left dot and n R electrons in the right dot. This two-electron system has four possible spin states: |S , |T + , |T 0 , and |T − . The |S ,|T 0 subspace is used as the logical subspace for this qubit because it is insensitive to homogeneous magnetic field fluctuations and is manipulable using only pulsed DC electric fields [12,13,15]. The relevant low-lying energy levels of this qubit are shown in Fig. 1c. Two distinct rotations are possible in these devices: rotations around the x-axis of the Bloch sphere driven by difference in magnetic field between the QDs, ∆B z (provided in this experiment by feedback-stabilized hyperfine interactions[16]), and rotations around the z-axis driven by the exchange interaction, J (Fig. 1b) [17]. A |S can be prepared quickly with high fidelity by exchanging an electron with the QD leads, and the projection of the state of the qubit along the z-axis can be measured using RF reflectometery with an adjacent sensing QD (green arrow in ...